1 00:00:01,486 --> 00:00:03,150 - [Voiceover] To change the speed of sound 2 00:00:03,150 --> 00:00:05,347 you have to change the properties of the medium 3 00:00:05,347 --> 00:00:07,629 that sound wave is traveling through. 4 00:00:07,629 --> 00:00:09,827 There's two main factors about a medium 5 00:00:09,827 --> 00:00:12,236 that will determine the speed of the sound wave 6 00:00:12,236 --> 00:00:13,473 through that medium. 7 00:00:13,622 --> 00:00:17,027 One is the stiffness of the medium or how rigid it is. 8 00:00:17,447 --> 00:00:19,928 The stiffer the medium the faster the sound waves 9 00:00:19,928 --> 00:00:21,384 will travel through it. 10 00:00:21,433 --> 00:00:23,334 This is because in a stiff material, 11 00:00:23,334 --> 00:00:25,646 each molecule is more interconnected 12 00:00:25,646 --> 00:00:27,546 to the other molecules around it. 13 00:00:27,652 --> 00:00:30,911 So any disturbance gets transmitted faster down the line. 14 00:00:31,204 --> 00:00:33,897 The other factor that determines the speed of a sound wave 15 00:00:33,897 --> 00:00:35,618 is the density of the medium. 16 00:00:35,632 --> 00:00:37,056 The more dense the medium, 17 00:00:37,056 --> 00:00:39,380 the slower the sound wave will travel through it. 18 00:00:39,555 --> 00:00:42,429 This makes sense because if a material is more massive 19 00:00:42,429 --> 00:00:45,685 it has more inertia and therefore it's more sluggish 20 00:00:45,685 --> 00:00:48,401 to changes in movement or oscillations. 21 00:00:48,401 --> 00:00:51,724 These two factors are taken into account with this formula. 22 00:00:51,973 --> 00:00:54,036 V is the speed of sound. 23 00:00:54,036 --> 00:00:57,316 Capital B is called the bulk modulus of the material. 24 00:00:57,511 --> 00:01:00,593 The bulk modulus is the official way physicists measure 25 00:01:00,593 --> 00:01:02,503 how stiff a material is. 26 00:01:02,719 --> 00:01:05,263 The bulk modulus has units of pascals 27 00:01:05,263 --> 00:01:07,721 because it's measuring how much pressure is required 28 00:01:07,721 --> 00:01:10,499 to compress the material by a certain amount. 29 00:01:10,594 --> 00:01:12,889 Stiff, rigid materials like metal would have 30 00:01:12,889 --> 00:01:14,814 a large bulk modulus. 31 00:01:14,814 --> 00:01:17,099 More compressible materials like marshmallows 32 00:01:17,099 --> 00:01:19,863 would have a smaller bulk modulus. 33 00:01:19,863 --> 00:01:22,092 Row is the density of the material 34 00:01:22,092 --> 00:01:24,381 since density is the mass per volume, 35 00:01:24,758 --> 00:01:26,836 the density gives you an idea of how massive 36 00:01:26,836 --> 00:01:29,281 a certain portion of the material would be. 37 00:01:29,445 --> 00:01:31,932 For example, let's consider a metal like iron. 38 00:01:32,281 --> 00:01:35,815 Iron is definitely more rigid and stiff than air 39 00:01:35,815 --> 00:01:38,275 so it has a much larger bulk modulus than air. 40 00:01:38,443 --> 00:01:41,006 This would tend to make sound waves travel faster 41 00:01:41,006 --> 00:01:43,026 through iron than it does through air. 42 00:01:43,250 --> 00:01:46,145 But iron also has a much higher density than air, 43 00:01:46,306 --> 00:01:47,782 which would tend to make sound waves 44 00:01:47,782 --> 00:01:49,262 travel slower through it. 45 00:01:49,319 --> 00:01:50,409 So which is it? 46 00:01:50,409 --> 00:01:53,069 Does sound travel faster though iron or slower? 47 00:01:53,218 --> 00:01:55,745 Well it turns out that the higher stiffness of iron 48 00:01:55,745 --> 00:01:58,419 more than compensates for the increased density 49 00:01:58,419 --> 00:02:00,498 and the speed of sound through iron 50 00:02:00,498 --> 00:02:03,631 is about 14 times faster than through air. 51 00:02:03,810 --> 00:02:05,034 This means that if you were to place 52 00:02:05,034 --> 00:02:07,936 one ear on a railroad track and someone far away 53 00:02:07,936 --> 00:02:10,499 struck the same railroad track with a hammer, 54 00:02:10,499 --> 00:02:12,997 you should hear the noise 14 times faster 55 00:02:12,997 --> 00:02:15,319 in the ear placed on the track compared 56 00:02:15,319 --> 00:02:17,508 to the ear just listening through the air. 57 00:02:17,708 --> 00:02:21,330 In fact, the larger bulk modulus of more rigid materials 58 00:02:21,330 --> 00:02:24,544 usually compensates for any larger densities. 59 00:02:24,707 --> 00:02:27,805 Because of this fact, the speed of sound is almost always 60 00:02:27,805 --> 00:02:30,864 faster through solids than it is through liquids 61 00:02:30,864 --> 00:02:33,699 and faster through liquids than it is through gases 62 00:02:33,787 --> 00:02:36,108 because solids are more rigid than liquids 63 00:02:36,108 --> 00:02:38,208 and liquids are more rigid than gases. 64 00:02:38,546 --> 00:02:41,358 Density is important in some aspects too though. 65 00:02:41,509 --> 00:02:44,257 For instance, if you heat up the air that a sound wave 66 00:02:44,257 --> 00:02:47,923 is travelling through, the density of the air decreases. 67 00:02:47,923 --> 00:02:51,442 This explains why sound travels faster through hotter air 68 00:02:51,442 --> 00:02:53,038 compared to colder air. 69 00:02:53,077 --> 00:02:55,345 The speed of sound at 20 degrees Celsius 70 00:02:55,345 --> 00:02:58,095 is about 343 meters per second, 71 00:02:58,095 --> 00:03:00,440 but the speed of sound at zero degrees Celsius 72 00:03:00,440 --> 00:03:03,802 is only about 331 meters per second. 73 00:03:04,252 --> 00:03:06,743 Remember, the only way to change the speed of sound 74 00:03:06,743 --> 00:03:09,812 is to change the properties of the medium it's travelling in 75 00:03:09,812 --> 00:03:12,769 and the speed of sound is typically faster through solids 76 00:03:12,769 --> 00:03:14,385 than it is through liquids 77 00:03:14,385 --> 00:00:00,000 and faster through liquids than it is through gases.